Hydrodynamics control shear-induced pattern formation in attractive suspensions
Dilute suspensions of repulsive particles exhibit a Newtonian response to flow that can be accurately predicted by the particle volume fraction and the viscosity of the suspending fluid. However, such a description fails when the particles are weakly attractive. In a simple shear flow, suspensions o...
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Veröffentlicht in: | Proceedings of the National Academy of Sciences - PNAS 2019-06, Vol.116 (25), p.12193-12198 |
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creator | Varga, Zsigmond Grenard, Vincent Pecorario, Stefano Taberlet, Nicolas Dolique, Vincent Manneville, Sébastien Divoux, Thibaut McKinley, Gareth H. Swan, James W. |
description | Dilute suspensions of repulsive particles exhibit a Newtonian response to flow that can be accurately predicted by the particle volume fraction and the viscosity of the suspending fluid. However, such a description fails when the particles are weakly attractive. In a simple shear flow, suspensions of attractive particles exhibit complex, anisotropic microstructures and flow instabilities that are poorly understood and plague industrial processes. One such phenomenon, the formation of log-rolling flocs, which is ubiquitously observed in suspensions of attractive particles that are sheared while confined between parallel plates, is an exemplar of this phenomenology. Combining experiments and discrete element simulations, we demonstrate that this shear-induced structuring is driven by hydrodynamic coupling between the flocs and the confining boundaries. Clusters of particles trigger the formation of viscous eddies that are spaced periodically and whose centers act as stable regions where particles aggregate to form flocs spanning the vorticity direction. Simulation results for the wavelength of the periodic pattern of stripes formed by the logs and for the log diameter are in quantitative agreement with experimental observations on both colloidal and noncolloidal suspensions. Numerical and experimental results are successfully combined by means of rescaling in terms of a Mason number that describes the strength of the shear flow relative to the rupture force between contacting particles in the flocs. The introduction of this dimensionless group leads to a universal stability diagram for the log-rolling structures and allows for application of shear-induced structuring as a tool for assembling and patterning suspensions of attractive particles. |
doi_str_mv | 10.1073/pnas.1901370116 |
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However, such a description fails when the particles are weakly attractive. In a simple shear flow, suspensions of attractive particles exhibit complex, anisotropic microstructures and flow instabilities that are poorly understood and plague industrial processes. One such phenomenon, the formation of log-rolling flocs, which is ubiquitously observed in suspensions of attractive particles that are sheared while confined between parallel plates, is an exemplar of this phenomenology. Combining experiments and discrete element simulations, we demonstrate that this shear-induced structuring is driven by hydrodynamic coupling between the flocs and the confining boundaries. Clusters of particles trigger the formation of viscous eddies that are spaced periodically and whose centers act as stable regions where particles aggregate to form flocs spanning the vorticity direction. Simulation results for the wavelength of the periodic pattern of stripes formed by the logs and for the log diameter are in quantitative agreement with experimental observations on both colloidal and noncolloidal suspensions. Numerical and experimental results are successfully combined by means of rescaling in terms of a Mason number that describes the strength of the shear flow relative to the rupture force between contacting particles in the flocs. The introduction of this dimensionless group leads to a universal stability diagram for the log-rolling structures and allows for application of shear-induced structuring as a tool for assembling and patterning suspensions of attractive particles.</description><identifier>ISSN: 0027-8424</identifier><identifier>EISSN: 1091-6490</identifier><identifier>DOI: 10.1073/pnas.1901370116</identifier><identifier>PMID: 31164423</identifier><language>eng</language><publisher>United States: National Academy of Sciences</publisher><subject>Computational fluid dynamics ; Computer simulation ; Condensed Matter ; Discrete element method ; Eddies ; Engineering Sciences ; Fluid Dynamics ; Fluid flow ; Fluid mechanics ; Hydrodynamics ; Mechanics ; Nonlinear Sciences ; Parallel plates ; Pattern formation ; Pattern Formation and Solitons ; Patterning ; Phenomenology ; Physical Sciences ; Physics ; Plague ; Reactive fluid environment ; Rescaling ; Scaling ; Shear flow ; Soft Condensed Matter ; Viscosity ; Vorticity</subject><ispartof>Proceedings of the National Academy of Sciences - PNAS, 2019-06, Vol.116 (25), p.12193-12198</ispartof><rights>Copyright National Academy of Sciences Jun 18, 2019</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><rights>2019</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c543t-59695ac7836c509784e7285b91bc24fe7986c15dfbe046230516b26efa80411c3</citedby><cites>FETCH-LOGICAL-c543t-59695ac7836c509784e7285b91bc24fe7986c15dfbe046230516b26efa80411c3</cites><orcidid>0000-0001-8323-2779 ; 0000-0002-4244-8204 ; 0000-0002-6777-5084 ; 0000-0001-5644-9905 ; 0000-0002-4706-885X ; 0000-0003-1845-2091</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/26743607$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/26743607$$EHTML$$P50$$Gjstor$$H</linktohtml><link.rule.ids>230,314,723,776,780,799,881,27901,27902,53766,53768,57992,58225</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/31164423$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.science/hal-02350009$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Varga, Zsigmond</creatorcontrib><creatorcontrib>Grenard, Vincent</creatorcontrib><creatorcontrib>Pecorario, Stefano</creatorcontrib><creatorcontrib>Taberlet, Nicolas</creatorcontrib><creatorcontrib>Dolique, Vincent</creatorcontrib><creatorcontrib>Manneville, Sébastien</creatorcontrib><creatorcontrib>Divoux, Thibaut</creatorcontrib><creatorcontrib>McKinley, Gareth H.</creatorcontrib><creatorcontrib>Swan, James W.</creatorcontrib><title>Hydrodynamics control shear-induced pattern formation in attractive suspensions</title><title>Proceedings of the National Academy of Sciences - PNAS</title><addtitle>Proc Natl Acad Sci U S A</addtitle><description>Dilute suspensions of repulsive particles exhibit a Newtonian response to flow that can be accurately predicted by the particle volume fraction and the viscosity of the suspending fluid. However, such a description fails when the particles are weakly attractive. In a simple shear flow, suspensions of attractive particles exhibit complex, anisotropic microstructures and flow instabilities that are poorly understood and plague industrial processes. One such phenomenon, the formation of log-rolling flocs, which is ubiquitously observed in suspensions of attractive particles that are sheared while confined between parallel plates, is an exemplar of this phenomenology. Combining experiments and discrete element simulations, we demonstrate that this shear-induced structuring is driven by hydrodynamic coupling between the flocs and the confining boundaries. Clusters of particles trigger the formation of viscous eddies that are spaced periodically and whose centers act as stable regions where particles aggregate to form flocs spanning the vorticity direction. Simulation results for the wavelength of the periodic pattern of stripes formed by the logs and for the log diameter are in quantitative agreement with experimental observations on both colloidal and noncolloidal suspensions. Numerical and experimental results are successfully combined by means of rescaling in terms of a Mason number that describes the strength of the shear flow relative to the rupture force between contacting particles in the flocs. 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However, such a description fails when the particles are weakly attractive. In a simple shear flow, suspensions of attractive particles exhibit complex, anisotropic microstructures and flow instabilities that are poorly understood and plague industrial processes. One such phenomenon, the formation of log-rolling flocs, which is ubiquitously observed in suspensions of attractive particles that are sheared while confined between parallel plates, is an exemplar of this phenomenology. Combining experiments and discrete element simulations, we demonstrate that this shear-induced structuring is driven by hydrodynamic coupling between the flocs and the confining boundaries. Clusters of particles trigger the formation of viscous eddies that are spaced periodically and whose centers act as stable regions where particles aggregate to form flocs spanning the vorticity direction. Simulation results for the wavelength of the periodic pattern of stripes formed by the logs and for the log diameter are in quantitative agreement with experimental observations on both colloidal and noncolloidal suspensions. Numerical and experimental results are successfully combined by means of rescaling in terms of a Mason number that describes the strength of the shear flow relative to the rupture force between contacting particles in the flocs. The introduction of this dimensionless group leads to a universal stability diagram for the log-rolling structures and allows for application of shear-induced structuring as a tool for assembling and patterning suspensions of attractive particles.</abstract><cop>United States</cop><pub>National Academy of Sciences</pub><pmid>31164423</pmid><doi>10.1073/pnas.1901370116</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0001-8323-2779</orcidid><orcidid>https://orcid.org/0000-0002-4244-8204</orcidid><orcidid>https://orcid.org/0000-0002-6777-5084</orcidid><orcidid>https://orcid.org/0000-0001-5644-9905</orcidid><orcidid>https://orcid.org/0000-0002-4706-885X</orcidid><orcidid>https://orcid.org/0000-0003-1845-2091</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Computational fluid dynamics Computer simulation Condensed Matter Discrete element method Eddies Engineering Sciences Fluid Dynamics Fluid flow Fluid mechanics Hydrodynamics Mechanics Nonlinear Sciences Parallel plates Pattern formation Pattern Formation and Solitons Patterning Phenomenology Physical Sciences Physics Plague Reactive fluid environment Rescaling Scaling Shear flow Soft Condensed Matter Viscosity Vorticity |
title | Hydrodynamics control shear-induced pattern formation in attractive suspensions |
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